SCIENTIFIC ABSTRACT SMIRNOV, L.P. - SMIRNOV, L.V.

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• Collection: Scientific Abstracts
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• Document Creation Date: November 2, 2016
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• Sequence Number: 16
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

S!'I:j,-C-,!, L. P.
Storage of powe-- cab7es. De--getfz-k I-, no. 12:'73-24 D T65
I - ~l
(,kfirA 19:1)
1. Glavrry inzhener kabel Inoy seti Mloskovskogo raycnnogo
upravleniya energeticheskogo khozyaystva.

SMIRNOV, L. S.
Smirnov,, L. S. -- "Process of Knitting Hosiery with a Covered Point, Eliminating
Looping." Cand Tech Sci, Moscow Textile Inst, 4 Feb 54.
( Vechernyaya Moskva, 25 Jan 1954)
SO: Sum 168, 22 July 1954

WIRNOV, L.S., kandidat tokhnicheskikh nauk.
Knitting hosiery products with closed too end without looping.
Ieg. prom. 14 no-7:17-21 JI 154. NLU 7-.7)
(Hosiery)

SMIRBDV, L., kandidat tekhnicheskikh nauk; SOKOIDV, V.
""Wwww'~
Some data on the knit-goods industry # German Democratic
Republic. Leg. prom. 16 no.1:54-55 Ja 156. JKLEA 9:6)
(Germany, East--Knit goods industry)

SMIRNOV, L.S., kand.tekhn.nauk
Specialization in Ukrainian S.S.R. knit-goods enterprises. Leg.
prom. 17 no.9:6-7 S 157. (MIRA 10:12)
(Ukraine-Knit
industr7)
goods

SMIRNOV, L. S., Imn,d. tekhn.
~
Impravo the knitting
n0.5:20-22 My '58.
nauk.
of hosiery with closed tips. leg. prom. 18
(Hosiery) (KiRA litO

S.iIRIUV, L.S.
Tricot witb tvio-sided raised capron nap. Tel-st.prom. 19 ilo.4:92
A-p 150, (Knit goods) (141RA 12: 6)

SMIRNOV, Leonid Ste-panovich: LIPKOV, I.A., kand.takhn.nauk, retsenzent;
F~ ~OVNT~Y,-F.H., red,; SHAPEITKOVA, T.A., tekhn.red,
LCircular maltiple-latch knitting machines] Kraglotrikotazhnye
mnogozamochnye mashiny. Moskva, Izd-vo nauchno-tekhn.lit-ry
RSFSR, 1960. 93 P. (MIRA 13:9)
(Knitting machines)

SMIRNOV, L.S.; ASPIR, B.G.
Manufacture of knit velveteen. Tekst.prom. 20 no-7:43-44
J1 160. (MIRA 13:7)
(Velvet) (Knit goods industry)

SL%I,IRI.'OV, Loonii,S_t~pppLnqy~q~_[Sfryrnov, L.S.1; KEiiSEK, Vladimir Nikolaye%40h
- -- [Kersek, V.14.1; LYASHCHENKO, T.V., red.; SMURTSMITEYN, K.A.,
tek-hn, red.
[1:e,,; goods from synthetic fibers] Novi vyroby z khimichnfth,
vaiokon. Kyiv, Derzh. vyd-vo tekhn. lit-ry URSR, 1961. 17 p.
(1-"IRA 15: ~)-
(Textile fibers, Synthetic)

WIRNOV, L.S., kand. tekhn. nauk; STAROVOYTENKO, G.P., otv. red.; TUBOLEVA,
..-M.Y.-)--,red.
(Artificial furl Iskusstvennyi mekh. Kiev, 1961. 39 P. (Obshchestvo
po rasprostranen'-iu politicheskikh i nauchrykh znnnii Ukrainskoi SSR.
Ser.6), no-15) (Fur, Artificial) (MIRA U'al)

alIRNOV, Leonid Stepanovich--GONTARERKO, Aleksandr Nikolayevich;
';a Georgiyevna; KRYLOV, Aleksandr Iosifovich;
NOVAK, Ilikhay Stepanovich; LYASHCHENKO, T.V., red.; STARODUB,
T.A., tekhn. red.
(Manufacture of artificial far] Proizvodstvo iskusstvennogo
mekha. Kiev, Gos. izd-vo tekhn. lit-ry USSR, 1961. 2,38 p.
(MIRA 15:4)
(Artificial fur)

SNIRNOV., L.S., kand.tekhn.nauk
Bulky yarns and their use in the manufacture of knit goods.
Takst.prom. 22 no.11:47-51 N 162. (MIRA 15:11)
1. Direktor Ukrainskogo nauchno-issledovatellskogo instituta po
pererabotke iskusstvannogo i sinteticheskogo volokna (UkrNIIPV).
(Yarn) (Knit goods)

.S-MIRNOV, Leonid Stepanovich; TRUMAN, Gennadiy Lukich; VINCH,
Lidiya Vladimirovna- DUBININA, Ollga Alekseyevna; KOBLYAKOVA,
I
Ye.B., kand. tekhn.nauk, dote.,, retsenzent; GABOVA, D.M., . I~Vl-
red.; TRISHINA, L.A., tekhn. red.
(Pattern design for knit goods]Konstruirovanie trikotazhjykh-
izdelii. Moskva., Rostekh12dat, 1962. 187 p. (MIRA 16:3)
(Knit goods) (Dresqmk4ng-Pattern design)

kand. telchzi. nwulr
1-'-anufacture of bi.C-k yarns and 1mit cyco-Js in the Tek~t. C- om.
24 no.4.--'-'--'-85
1. ~irektcr likrainskogo iir--ucLn(,,-.i-,c;s,e.~ovatellskooo no
F11-reT."~v'O'n !"Skusstvennykh i 3intcticheckikh volok-o-

PIGALEV, A.V.; SMIRNOV, L.P.; le,,A.
Modification of the arrangerent of co-Lton bales in .1 ront oi' the
breaker unit in case of the increase of their munber. Tekst.prom.
25 no.2:42-43 F 165. (MIRA 18:4)
1. flachallnik pryadillnogo proi,,,vodstva No.1 Kherson-,,.kogo
khlopchatobm-izhnogo kombinata (for Pigulev). 2. Nachallnik
sortirovoohno-trepallnogo tsoPhit pryaldillnogo proiz,.md.~Jva
No.1 13ior.Tonologo linmh1w:tt~m (for Irt 1 e-v)
3. Stivrshi,,r inzh. labor~thjrii ixvii(IIII11opo

S'L,17 '.ICI'7 ' 'I
HI ~y 1-0., fl-aEd. te:di. nauk; I.I.V.
Characteristics of the techrology of knit goods manufacture
from bulIzed loop yarn. Leh. prom. no.4:7-9 O-D 165.
(Iff"'k 19; 1)

kand,tekhn.nauk; KALECHITS, I.S.
Charac terts tics of the technology for the manufacture of man's
socks from bulked loop yarn. Tekst.prom. 25 no.11:48-51 N 165.
(MIRA 18:12)
1. Direk-tor Ukrainskogo nauchno-issledovatellskogo instituta po
pererabotke iskusstvennykh i sinteticheskikh volokon (UkrNilpv)
(for Smirnov). 2. Zaveduyushchiy sektorom trikotazha laboratorii
obl'yemnykh nitey Ukrainskogo nauchno-issledovatellskogo instituta
po pererab'tke iskusstvennykh i sintaticheskikh volokon (for
0
Kalechits).

L 441Q-66 Exf W/ J)IT-- _RM
ACC NR: AP6021367 (4) SOURCE CODE: UR/0342/66/000/003/0071/0072
AUTHOR:- Smirnov, L. S., (Director, Candidate of Technical Sciences);
Polokhova. S. S. , (Senior Research Associate)
ORG: Ukrainian Scientific Research Institute for the Processing of Artificial
and Syni-h-etic Fibers. [UkrNITIPV] (Niauchno-issledovatell skiyinStitut po perira-
botke iskusstevennykh i sinteticheskikh volokon)
TITLE: Some physicomechanical properties of bulked yarns
SOURCE: Tekstill naya promyshlennost' , no. 3, 1966, 71-72
TOPIC TAGS: bulked yarn, chemical filament, banlon fiber, elastic fiber, meron
fiber, fluflon fiber, agilon fiber, spun fiber chemical fiber, crimp
ABSTRACT, The article describes tests made to determine the amount of crimp
and the elasticity of various types of bulked yarns, including fluffy, elastic, and
meron yarns from the USSR and banlon, fluflon, agilon, and spun yarn from the
USA. The amount of crimp was determined by a method de veloped at the Central
Scientific Research Institute for Wool,KMINIIShersti) mentidned in another work
1/2 UDC: 677. 494. 001. 4

7
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therinal exO. -were measured ~ 1~y ~iht_ m___ of coutch-
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Quantitatively avalti~tcd it the Me of the variom parts f
the swface-.:of -. the ~ m1conductor In the crmflon o the,
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-at be obtained aftesoue or the other sutface treatmcnt if
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If -7:

SUBJECT USSR P11YSICS CARD 1 3 PA - 1377
AUTHOR _-WASILO'J"', -J,3. ,S1,11IMM71', L. S. , GAU111, G. ISPIZYN, A.V1. ,
PAME'Vild, -'I':. M_
TITLE The Fornation of Defects on the Crystalline Lattice in Germani.-am
on the Occasion of a Bombardment by Fast Electrons-
PERIODICAL turn.techn.fis, 26, fasc. 9, 1865-1669 (1956)
Issued: 10 / 195-6 reviewed: 10 / 1956
The purpose of the present work was to clear up the dependence of the croS5
sections of formations of defects of the FRENKEL type on the electron eneraies W
and to find out how many energetic levels, that are connected with the afore-
mentioned structural defects of the crystal, influence conductivity. Experiments
were carried out in the course of which the mcnocrysts.13 of germanium with an
elec tron conductivity were bombarded with monoenergetic electrons
;1 < 8~) of an energy of from 400 to 1000 keT. Electron irradiation and the
W
0
following measurements were carried out at room temperature. Thin (CO/A ) mono-
crystalline plates were used, The energy loss in them amounted to not more than
60 keV. Three different methods were employed for measuring the specific re-
sistanGe q of the irradiated crystals: 1.) A homogeneous crystal with a known
initial specific resistance Q0 was bombarded with electrons that impinged upon
a surface of the greatest area. The resistance of the sample was measures) where-
upon a layer having a thickness of 50/" was ground together with the bombarded

V
Zurn.techn.fis, 26, fasc. 9, 1865-1869 CARD 2 / 3 PA - 1377
surface and the resistance of the remaining part of the crystal was measured.
From the distance between resistances the resistance of the part which was
.-round together was determined. , Herefrom its specific conductivity Q after
bombardment was computed,
2.) A homogeneous crystal was bombarded as described under 1.) and then its
bombarded surface was pasted on to a glass by means of Canada balsam where I't
was ground together to a 'thickness of 50,0-The resistance of the thin remaining
plate was then measured.
3.) The resistance of monocrystalline plates with a thickness of 50 AE, , which
were pasted on to glass, was measured, whereupon they were bombarded with ele--
trons. The resistance was then newly measured.
7,'hen measuring the resistance of thin crystals of germanium it is always
necessary to reckon with the possibility of the formation of surface layers
.iith increased resistance, The experiment showed that the threshold value of
the energy Wmin' from which onwards the conductivity of germanium crystals
diminishes by irradiation, is equal to 500 + 20 keV, The results obtained by the
present work are not in contradiction to the hypothesis of JAMES and LARK -
HORWITZ if it is assumed that a donor level of the defect and an acceptor
are near -the corresponding zones. (The hypothesis says that to an atom in the

SMIRNOV, L.S.
"Energy of Ionization by Beta-Particles in Crystals of Germanium and
Silicon," V.s. Vavilov, L.S. Smirnov, V.M. Patskevich, Moscow, USSR
Paper submitted for presentation at the International Conference on
Radioisotopes in Scientific Research, Paris, 9-20 Sep 1957
Acad. Sci. USSR, moscow
Presented at Conf. by V. s. vav-_jjv

SMIRNOV, L.S.
"The Structural Defects in Germanium Monocr-fstals Irradiated by Beta-
Particles and Fast Neutrons and the influence of These Defects on -Electron-
Hole Recombination," V.s. Vavilov, L.S. Smirnov, A.V. Spitsyn, V.M.
Patskevich, M.v. Chukichev, Moscow, USSR
Paper submitted for presentation at the International Conference on
Radioisotopes in Scientific Research, Paris, 9-20 Sep 1957.
Acad. Sci. ESSR, Moscow
Pre5ented at Conf. by V. S. Vavilov

AUTHOR VL~ B.M. ~ VAVILOT4 V. S. 9 SMIRNOV; L. S 4
GALKIlt, G, N. g PATSKETICE1, Y-M. -I
SPITSYN,,A.V.
TITLE On 'the transformation of the energy of P-particles int3
electric energy in germazium, crystals with P-N transitions.
(0 pTeobrazovanii energii P-chastits Y electroenerglyla T
kristallakh germaniya s P-N-perekliadazil,- Russian)
PERIODICAL Atomnwja Energiya 1957P Tol 2, Nr 6, PP 533-537 (USSR).
ABSTRACT In "955 thp authors carried out experiments in the deter-
mination of the degree of efficiency of the transformation
mentioned in the title. The P-N transitions were obtained
by the melting of indium. Sr90 - Y90 preparations ser-yed as
sources of P-particles. The total activity of the primary
radloacti-re preparations amounted to 50,100, and 200 inilli-
auxies, As source of P-particles strontium sulphate tablets
with 50 and *iOO millicurie and stroatium carbonate tablets
with ?00, millic-urie were used. A diagram shows the P-spectra
of these sources. Also measurements during irradiation of
a ssmisonduG-tcr with artificially accelerated electrons (400
to 1150 keV) were carried out. Zte degree of efficiency
CARD 113

24
On the transformation of the energy of P-particles
into electric energy in germanium crystals witk P-1 transi-
tions~
the degree of efficiency of the transformer dimialskes.
Further details are mentioned.
(With 6 Illustrations)
ASSOCIATION. not given.
FRUENTED BY: -
SUBMITTED: 18~4j- 1957-
ATAILABLE: Library of Congress.
CARD 3/3

PA - 2148
Probabilit) of Charge Carriers by Frenkel Defekts in
N-Germanium.
restitution of the original life. If the number of defects
,pecuring in the chrystal lattice is compared with the
L
-attendant circumstance of reduction of life the capture
cross-section )f the carriers (holes) can be estimated
(by the new-formed recombination-centers). The formula for
the capture crdss-section is derived on the assumption that
the number of new recombination-centers is equal to the
number of Frenkel-defects and that all these centers are
filled with electrons. Experimental result for this domain
which must be considered to be the lowest of the actual
value, were approximativelY 7-10-17cm2. (I image).
ASSOCIATION: Physical Institute "P.N.Lebedev", Moscow.
PRESENTED BYs
SUBMITTED: 1.10-1956
AVAILABLE: Library of Congress.
Card 2/2

AUTHOR: Smirnov, L. S. 57-11-7/33'
TITLE: Measurements of Small Lifetimes of Current Carriers in Germanium
(Izmereniye.malykh vremen zhizni nositeley-zaryada v germanii).
PERIODICAW Zhurnal. Tekhn. Fiz., 1957, Vol. 27, Nr 11, pp. 2469.247,1 (USSR).
P
AMTRACT." For the measurements types in form of small germanium plates with a
y&ep-transition, on a great surface were used. Nonequilibrium, carriers
were excited by monochromatic light in vicinity of the semiconductor
surface. The lifetime of the current carriers was computed according
to the short circuit current and the number of the absorbed, light
quanta. Applied to germanium this method facilitates the measuring
of a lifeti*e of from. 2.&ln-6 to lo-4 see. This method is ver7- praeft
tieak for the detection of the temperature dependence of the life-
time and for the determination of the position of recombination lea
vols. Formulae are derived by meanB of which the lifetime in the
semiconductor layer can,be determined experimentally by determinan
tion of the quantity&&,,aCn, is the ratio of the number of carriers
which take part in the short circuit current I to the cumber of
carriers N which develop by the light in the vicinitd-6t:the semi-
Card-1/2 conductor surface within the time unit,,.The,mentioned formulae effect

ni VO V/
IMIR/Electricity Semiconductors G-3
Abs Jour : Ref Zhur - Fizika, No 1, 1958, 1325
Author : Vavilov, V.S., Spetsyn, A.V.; Smirnov, L.S., Chukichev,
M.V.
Inst : Fhysics Institute, Academy of Sciences, USSR, Moscov
Title : Effect of Fast Neutron Irradiation on Recombination of
Electrons and Holes in Germanium Crystals.
Orig Pub : Zh. eksperim. i teor . fiziki, 1957, 32, Ito 4, 702-705
Abstract On the basis on the transverse cross sections for the
interaction of fast neutrons with germanium nuclei, using
the Snyder and Neufeld method (Referat Zhur Fizika, 1956,
Ito 7, 1984o, Ito 12, 35072), the authors calculate the num-
ber of germaniim atoms, shifted from their lattice points
as a result of scattering of fast neutrons. It was esta-
blished experimentally that the irradiation of germanium
Card 1/3

AUTHOR VAVILOV,V.S., SMIRNOV,L,,S., PATSYX-VICR,V.bJ. PA - 2332
TITLE: Energy of Ioni ion by Electrons in Germanium crystals (Ener-
gyya ionisataii elektronami v kristallakh germaniya, Russian).
PERIODICAL: Doklady Akademii Nauk SSSR, 1957, Vol 112, Nr 6, pp 1020 - 1022,
(U.S.S.R.)
Received: 4 1 1957 Reviewed: 5 / 1957
ABSTRACT; The authore carried out experiments on the determination of the
average ionization energy in germanium on the occasion of ex-
citation by electrons with 5 - 15 keV. For these experiments
N-Type crystals with P - N - transitions, into which indium was
melted, were used. Irradiation occurred on the side opposite to the
indium electrode. The electronscompletely lost their energies with-
in the domain of the N-type. The authors used the following de-
notations: N 0 - the number of-carrier pairs actually created in the
unit of time, N I - amperage of the electrons, N amperage of the
holes. It holes that 'B 1 = K 2/"l 12/1 where corresponds
to the primary current corresponding t~'the flux"of the fast
electrons. Up to very high intensities of the inciting bundle it
further holds that N 2 = o(N . Due to recombination on the surface
and in the interior of the crystal it always holds thatch< 1. For
the multiplication factor B it holds that 8 0 N IN B /0(
I /,yI1, In the case of the crystals examined &4 did n3t de-
Card 1/3 ;ena on he wave length of the light. This holds good up to such wave
Energy of Ionization by Electrons in Germanium crystals.
PA - 2332
wave lengths in the case of which a considerable part of the light
does not pass through the crystal but is absorbed in it. For the
measuring of o(the authors used light with ~- 1~05 ~L which for
the most is absorbed in layers with a maximum thickness of I,O~L -
rX depends greatly on the conditions prevailing on the surface of
the crystals and changes on the occasion of the pumping out of the
device and of bombardment with electrons. For the purpose of a
continuous control ofcX in the course of measurements, the glectrone
were at the same time irradiated with electrons and bight. The
tests were carried out at pressures of lo-4 - 2.10- torr.No
dependence of E (i~e. of the energy which must be used for the
production of a carrier pair) on pressure (within the limit,3
2.10- 6 _ 10-4 torr) was noticed. The series of measurements on
the crystals, which were subjected to different surface treatments,
furnished the same value for The mean value 3t7 � 094 ev
was obtained from 4 series of measurements. In the case of V " 5
to 15 keV E does not changed This indicates slight energy losses
of the primary electrons in the superficial oxide film which
occurs on the occasion of the pickling of the germanium. The con-
siderable similarity of the amounts of F on the occasion of
Card 2/3 ionization by electrons and X particles may apparently be ex-

PA - 2332
Energy of Ionozation by Electrons in Germanium Crystals.
plained by the fact that in the second case a considerable
part of the charge carrier pairs occurs under the effect of
relatively fast d-electrons. (1 illustration)
ASSOCIATION: Not given.
PRESENTED BY.- Member of the Academy D.V.SKOBELITSYN.
SUBMITTED: 24-10-1956
AVAILABLE: Library of Congress.
Card 3/3

AUTHORS: Vavilov, V. S. , dMjrAw~. ~.~itayn, A. V-~ 57-28-5-6/36
Patskevich, V. hT., Galkin, G. 11.
TITLE: On Defects in a Crystal Lattice in n-Germanium (0 defektakh
kristallicheskoy reshetki v germanii 11-tipa)
PERIODICAL: Zhurnal Tekhnicheskoy Fiziki, 1958, Val. 289 Nr 5, pp. 96o-
-961 (USSR)
ABSTRACT: In the previous paper the authors communicated the investigat-
ion results of germanium crystals of the n- type subjected to
an electron bombardment with energies ranging from 0A to 1 MeV
(Ref 1). There, the experimentally determined modifications
of the specific resistance with respect to theJenergy and the
amount of fast electrons, was opposed to the theory of defect
formation because of an electron dispersion by means of ger-
manium nuclei by Frenkell. V. V. Galavanov to whom the authors
are indebted, indicated a num~~rical error. This error was
committed in the computation of the integral aoss-sections
of electron dispersion on a nucleus at all angles from n to &min
the angle Amin at which the electron transfers the minimum
energy to the nucleus neceasary for the formation of a defect.
Card 1/2 The newly computed theoretical values of :~M:in correspofiding to

On Defects in a Crystal Lattice in n-Germanium 57-28-5-6/36
a threshold energy of 500 keV as well as the experimentally de-
termined sectionsZ of center formation, which remove the elec-
trons from the conduction zone are given in the table. From
this follows, that the experimental values, which have been
obtained in the mentioned paper and which were verified by
subsequent experiments, do not correspond to the conception
that at energies W varying from thekhrenhold energy (W -0,5 MOV)
to W - o,96 MeV the constant defects in n-type germanium are
produced according to the law � =f (W)
@min
It is intended to conduct in the near future experiments with
n-type crystals with strongly differing Fermi levels and to
determine, whether the difference between theory and experi-
ment is dependent upon the low de,-ree of filling of the capture
centers. There are 1 table and 1 Soviet reference.
ASSOCIATION: Fizicheskiy institut im. P. N. Lebedeva AN SSSR, Moskva(Physicr.1
Institute imeni P. N. Lebedev AS USSR, Moscow)
SUBMITTED: J'anuary 18, 1958
Card 2/2 1. Germanium crystais--Anal~rsis

1'?") 00 67391
CK SOV/181-1-9-9/31

AUTHORS: Smirnov, L. S., Glazunov, P. A..
------------------------
TITLE: The Spatial Distribution of Lattice Defects in Germanium
Crystals~lrradiated by Fast Electrons -1k
Y

PERIODICAL: Fizika tverdogo tela, 1959, Val 1, Nr 9, pp 1376 - 1378 (USSR)
ABSTRACT: The aim of the work under review was to investigate the
spatial distribution of the lattice defects due to electron
irradiation by measuring the electrical conductivity in the
direction of the electron beam incidences figure 1 shows a
scheme of the experimental setup. The measurements of con-
ductivity were made every 10 - 50,1?,with a probe by the use
of a PPTV potentiometer. The defect concentration was .
sufficiently small so that every change in conductivity was
due to a change in the carrier concentration-'\n orzNp.z~n is
proportional to the defects produced. They~~n distribution in
the sample interior must therefore correspond to the
distribution of the structural defects, if the properties of
the defects do not depend on the electron energy. Surface
influences can be eliminated by a corresponding choice of the
Card 1/3 sample dimensions~ The dimension selected for p- and n-Ge vFa
---------- I

67391
The Spatial Distribution of Lattice Defects in Germanium SOV/181-1-9,:-~9/31
Crystals Irradiated by Past Electrons
assistance in measurements There are 3 figures and 2 Soviet
references.
ASSOCIATION: Fizicheskiy institut AN SSSR im. P. N. Lebedeva Moskva
-(Physics Institute of the AS USSR imeni P. N. Lebedev,Moscow)
SUBMITTED: March 7, 1959
Card 3/3

B-Z556 01 /041
BoP
'Boo6
69-1610
6 t1K
00 '4 JAO. I es
-2S'
o PTO'P t1le
-qO1
A960s sses
ion 13 J 11
t114w~G a a iscu ,aTament
~'at'ho ts -bos t-his
tve-ra0go 8.1fleots tyke to I t ivL
TIT -I'S ticles Or ~,bou.
t -pap t 8.1 8"'0 -t~t "cupy a
aL 0
jast -par rese-A Cris b'roug 5
the 9 s T esult
r t O-f aTe S.1 t e a all then
t-101L aLjec' s Ut al
tutbsXlce %hei- Time tion IS it tile
-a V-fl)e
-L;E-erabIl 0, limp Ong -
Of Ja t.~ce JOB+. -grate j:-r~ es) er a 9 10 e
O*a TtLe Sisq evapo canol 0.+couditl
atoms I -qs t ~kna of some
a CTI tajo Of ,,Ge'P * er siler 9 O-re tban
e ana jetAT t1la e%P all JOT
su%e ~j OT 3.9 3 the ires Or ea, up
%~rq f asl as n0aes t 10it ,it I acq'11 ace .e Odiate
vitb ()ne ma tyLe 6 Son %teTttc e, i.% S'01 IS into
case. 6e T i; 0.4er
e betileeU C,.r ag 'Onie ST r from e-ne' .11 pass
01 f
_ao 3.n sea 9 gat
I . iT eO~E 0 a
POUTY Ga 04 Va a ao-qe e,, . son
aT e '611 ais - il-.i't9 t j:ix 11 -r 6 93-
-r"'ag 01.1isio" obau aJ%O 5 ~'f-feot" gza
tho aYL eat!%19' an(, tais
a-to%v nst a-at a eLl 9
Thl
v ~11 0
Je. 06 ttice
T t e atom.
lae 0
T~e illoo
.a A
82556
S/WJ60/002/007/041/042
Radiation I)isturbaw-es in crystals B006/Bo6o
61 to local
~n melting are 'posed ureg atoms
Substances that expand c r this press
2 a result 01 vhen ffio'lteng
104 kg/cM . As xhib it, f or
the Molten state. e yrystals e example,
es of the ord ,,,,,d region. Some vh-lchg Dlume. The
itted in the order Of their atoms-,ease in V'
s rsh ort-range , [ germanium to a dear e order due both to
may k a]
PrOs b : in the sh Id rbance of th ;tq5mp+,s to
a 'va ia he case Of "'Oor Of a distu order. Tile author ILI anium, the
leads in t defect thus Consists shoTt-rangO For germ
radiation on in the he purpose one atomic
p 98sure and variati energy necessary for t ed for breaking
minimum energy requil -rough estimationg
r 4. imate the he a -very is equal
e 8 4 .. 38o kevq and if t' it is found, in y be T.-arranged
minimum 3- Sgumed to be o,6 evq the jar mE ound for silicon. If nd-
bond is )lume in 'which Or~ions are f shifted depe
smallest 'v' milar condit Iergy is
ing 6l,
that the )-jume Of 26 atoms- Si,orreot the limit 1 woo e . If one irradiation
to the V1 esed here are 0 ion takes Poo C higherg the limit
the ideas discu h irradiat other at 2 author f inallY
On the temperature at _*hc,,ture and an
ing . room temper, 20 30 kev. The
is carried out al can be shif ted by
energy Of germaniU% for .,-,is discussion.
thanRs V . S. Va-vi1O
C.
Card 2/3

33096
S/638/61/001/000/0!9/056
-it, ~700 (IOL13 B104/B!38
AUTHORSt Smirnov, L. S., Glazunov, P., Ya.
TITbEt Volume distribution of lattice defects in germanium crystals
irradiated with fast clectrono
SOURCE,- Tashkentskaya konferentsiya po mirnocV ispol~zovaniyt~
atomnoy energii,, Tashkent, 1959. Triidy, v. 1. Tashkent, 1961,
153 - 155
TEXT: The determination of defect concentrations in Ge crystals was
based on the relation between the defect concentration and the concentra-
tion of additional acceptor centers. The variation in the conductivity of~/
irradiated crystals was studied by taking the potential distribution
(Fig. 1) with a probe at intervals of 10 - 50,-, The defect concentration
was so low that it did not affect mobility and the entire variation in
conductivity was due to variation in carrier concentraticns, The n- and
p-type germanium samples had dimensions of 1.0-3.0,5.0 mm, and Y o =
10 - 15 ohm-cm and 40 - 50 ohm~cm, respectively. The samples were irradia-
Card 1

:1,769 o1/056
11-1/003/011/0
-aOv t
-Ir
jr
aiate&
lavilo IT, P_ type neutr 0,,-Irra
2lotn"Ov' vit
1,~jjletics Of photocon&ucti 1961, 3-53 - 3259
silicoll no. investi-
T IT LS v. 3 1 , beell
telav troll irr &ia'!11uS.& had-
,,7,i,,, tver&Ogo to f ast-riwa s eciluells The
The 1 61)-. the
&ue
I)F IOVIC -L' sil-jcOn. tioa 3.11
(?TT
formation p.;tyqe paper rirra JEL V
-11 tivit tiga,
&erect r1 er inves,
eut
Tile ingle crystals Of all e a e fas Ile vels .,+,.30 e
colld-
TSIT' in S thorB ill ~ to Oto e 1e elec-
gate& th e ala d6u( 8 0, to The
ri5ing . 1. sit! 0Y,
bed6 by teM a .F-1g. or
d.escri I SYS wn 3-11 ctr - around, 100 times
. leve . sho electr
defect ban& IS I . th -the e Was e and. aec&Y f or each
fOrbi&&e'acOjj-aecte& W1 Temperatar w i th ris aratelY &Pbll
s that + o-45 e"V ses . &sep , time
5 tud., e. 1d-111
wa ev alla. Bv oa. light '911 -was v. TDV '0111 OscillOBcOP e-
+ steep, axatioll
C).38 -SI I
te& by uction re S + 0.30 e (Yso A
troll was e%ci ?hotocoll methods' IV '90 orl all
~jsec each' in&epenclent f ouna at & p
5 two ty Vlas
level ocoll &ue t-1,V3.
of pho
Cara. 1/4
6
5/181 3TJ11003/011/ool/056
B102/B138
Kinetics of photoconductivity in s found to be
m I the initial electron concentration at level M, wa trapping
0 12 -3 *3 '10- 14cm 2 was determined for the hole
10 cm and d P _f(t) were investigated for
section. (2) The build-up curves&Pbri erned by an 9XPO-
cross It was confirmed that the building is 90v P41013CM-3,
PO).&P. The parameters of the centers were found to be Mo -14 2
nential law. 2 and m1,;-410 13CM-3 9Lf W2-5 ' 10 cm
0 14 3 '10 -14cm (first illumination) (1) Recording of pthe relaxation
p liumination) . Ev + 0.38 ev: 8-3 &PP43- 108CM-3
(second i ant illumination for Potri 8 - 10 cm and
pulses without const _ 3 -1 .0-17cm 2. (2) Recording Of,&Pb,
m qI/v10 9cm - see and d A15 1 10 Scm-3) yielded.:
yielded: 0 1:4 6 - lp 9CM-3 and 6 p 14 3 *
with constant illumination (po , 0 2. (q - capture cross section
9 -3 R$7 - 10 ::17cm
M CjIrj10 cm see and Cf p I - intensity of exciting
0 ton by an ele'Otron at the level M; 'of time. it was
of a pho was studied as a function
light.) E + 0.45 ev: &Pbn V+ 0,30 ev
found thatvfor t /_ 0.2 sec carriers localized at centers with F
Card 2/4

10~ 69
S 181/61/003/011/001/056
Kinetics of photoconductivity in ... B102/B138
for remarks, critics and help. There are 10 figures and 5 references:
4 Soviet and 1 non-Soviet.
ASSOCIATION: Fizicheskiy institut im. P. N. Lebedeva AN SSSR Moskva
(Physics Institute imeni P. N. Lebedev AS USSR, Moscow)
SUBMITTED:, April 29,1961
Fig. 1 Ic
tie
Card 4/4

L-ogo4
S/1 6 1/62/004/bO9/044/b45
B104/B166
AUTHORS: Smirnov L S Vavilov, V. S., and GeraBimenko,. N. 11.
TITLE: Kinetics of silicon recombination radiation
PERIODICAL: Fizika tverdogo tela, v. 4, no. 9, 1962, 26n-2629
TEXT: The possibility of studying the kinetics of silicon recombination
radiation is examined. Rectangular current'pulses were fed into Si
crystals with p-n junctions. The recombination radiation from the
crystal was taken by a photonultiplier, ahplified.with a broad-band
arrt)lifier and observed with an oscilloscope. The:crystals had~been
produced by diffusion of phosphorus and by fusing alumInum on to the
surface." The injection coefficient was assumed to remain constant up to
current densities of 10 a/cM2. Results; The attenuati*on of recombinAtion
luminescence can be well described by an exponential law. The time
constants of att*enuation are approximately 2.7 microseconds for crystals
with diffused junctions, 1.5 microseconds for crystals with fused
june tiorrs. When the crystal is cooled to liquid nitrogen temperature the
pulse amplitude does not decrease in proportion to the change in the
Card 1/2

S/181/62/004/012/016/052
The theory of radiation defect ... B104/B102
NA
NA (NA vw-G"
(7)9
P.
can be written in the'form f 1/(At+l). If A is chosen suitably,
curves obtained from (7) agree fairly well with experimental data
obtained by W. L. Brown and W. 11. AngUBtyniak (J. Appl. Phys., 30, 1255,
1959) and by G. Bemsky and W. M. Angustyniak (Phys. Rev., 108, 645, 1957).
There are 3 figures.
ASSOCIATION: Fizicheskiy institut im. P. N. Lebedeva AN SSSR Moskva
(Physics Institute imeni P. N. Lebedev AS USSR, Moscow)
SUBMITTED; juiy 6, 1962
Card 4/4

3 6 o 3 0'z 0 0 1 G 0
t~ 1 10
.iUTIHOP.: Alikhanov, F,. A. L. S.
ORG: none-
TITLE: Nceutrono-raphic investigation of 'the low-temperature magnetic transiti
in chroniium
SOURCE: USSR. Gosudars-4vennvy ko-znitet Po -,'spoPzov3.i-,iy-,1,, atomnoy energii.
L L -ezro o-
Insti'u~ tcoro'iches'~,.)v c-"~SOCZ-~MC'- !iZild. DO-.k OG--, r
-0. N
nizkotempo-raturnogo ma-n-`nogo prevrashclieniya v
rzhrome 1-15
TOPICTAGS: chromium, cryostat, lowternperature
ma,gneLictranslt4on, crystal spin structure, chromiumcryszal, neutron scattering,
magnetic scattering
ABSTRACT: A s'-iciv v.-a;3 madQ of the 'ow-t(-m,)erature maune~ic
t - a n s ii i-~ Of ~alll ,c chromium con
-hanical
z a. I he
~reaz~ Z 0 -~i ~;j--j mn was use
Card 2

ACC N'Ri
SLudy showed that the transition temperature 'A7'Fq increases ar, -increase in
metal plasticity, and that the spin density moduiation period, and its temperature
dependence are a universal property of chromium. The authors 'thank P. L.
Kapits for 'his interest in this work and 1. 0. Panasyuka, D. D. Abanjn, T. !.
Kostin and T. 1. Xozlov for their assistance. Orig. art. has: 5 figures.
[Authors' abstract]
SUB CODE: 20/ SUBM DATE: none/ ORIG REF: 009/ OTH REF: 0091
2

jZ.U6_-A6Lr_ )/EWP(t) TJT
- - AP6_JM)_;'/rfiT(1)ZRWT( SOURCE CODEIUL
ACC NR,, - UR70 0a76A2/0603/0Zb5
A6OR: Vasil'yev, A. V.; Smirnov. L. S.
ORG: Institute of Semiconductor PhysicsSO AN SSSR,_Novosibirsk (Institut fiziki
poluprovodnikov SO AN SSSR)
TITLE: Infrared quenXing of the natural photoconductivity in n-type germanium.,
irradiated with gamma raXs
SOURCE: Fizika tverdogo tela, v. 8, no. 2, 1966, 603
TOPIC TAGS: gamma irradiation, photoconductivity, germanium semiconductor,
germanium.single crystal
ABSTRACT: An investigation was made of the.photoconductivity in n7type germanium
irradiated with gamma rays from a Co" source at room temperature. The specimens
were cut from an ingot of n'-type germanium.with a donor concentration of -.1014 cm73.
In a series of irradiated specimens the initial donors were almost totally compen-
sated by acceptor centers introduced during irradiation. The following system o
radiative defect levels in the forbidden zone was determined from the photoconduc-
tivity spectrum taken at the liquid nitrogen temperature: EC-O.~22,1-0.25, -0-27,
-0.30, -0.33, -0.36, -0.43, -0.49, -0.52, and -0.59 ev. The conductivity in
its natural range was quite inertial. Its rise up to a stationary value took CU12 sec;
its decrease took 1v10 min. At constant illumination an infrared quenching throughout
Cc.i-rd-- -1/2-

ACC NR; AP6006866
virtually the entire investigated range of wavelengths (1.5-5.5 v) was observed In
specimens compensated during irradiation. The quenching spectrum showed three
clearly distinguished quenching maxima at 0.47, 0.52, and 0.60 ev. A weak quenching
was also observed in the region of 0.2-0.4 ev. The results obtained apparently,
follow from a series of defects with different -cross sect-ions,ft electron and hole
capture produced by irradiation. The quenching maxima at 0.47 and 0.52 ev can be
attributed to the transfer of electrons initiated by infrared light from the valence
zone to the EC-0.27 and -0.22 ev levels, respectively. The maximum at 0.60 ev
shows the presence of the E -0.14 ev level in the forbidden zone. Orig. art. has:
1 figure. C [JAI
SUB CODE: 20/ SUBM DATE: 09Apr65/ OTH REF: 001/ ATD,PRESS: C/ 0
ard 2/2 not

AP6012492 SOURCE CODE: UR/0181/66/006/0011/1246~12119
LC
~IAUTHORS: Geytsi, I. I..; Nesterov. A. A.; BarinovA, E. Yu.; 4pirno~,,_
IL. S.
ORG: Institute of Semiconductors,,SO.AN SSSR,Novosibirsk__(I stitut 73
poluprovodnikov 7.) AN SSSR)
TITLE: Temperature dependence of the average ionization energy In
germanium and silicon
SOURCE: izika tverdogo tela, v. 8, no. 4, 1966, 1246-1249
TOPIC TAGS: germanium, silicon, ionization, temperature dependencej
electron bombardment, x ray irradiation, photoelectric property,
physical diffusion, minority carrier, forbidden band2 G-Fe'.."'F9 A-# O"L
'r14-1C6AJ -5'P'n(42dA.)JDLJ4Cr4,0e -:?
ABSTRACT: To obtain additional data on ionization occurring in 4mi-
conductors irradiated with electrons and x rays, the authors measured
the temperature dependence of the average ionization in Ge and Si. The
relative change of the ionization energy with temperature was determined
by two procedures. X rays were used for uniform generation of carriers
in the volume of the semiconductor and to avoid the influence of irradia
tion on its surface propertiesi The x rays range in energy from 30 to
50 kev. The x ray pulses ranged in duration from 10 to 500 ~Lsec, with

-L 46831-66 w)/EWP(t)/ETI/T . IJP (C) JD/AT
ACC Mt AP6015464 (V SOURCE CODE: UR/0181/66/008/005/146f/1466'
AUTHOR. Gerasimenko, N. N.; Loburets, Yu. V.; Polyakov, G. F.; Smirnov, L. S. 4
ORG: Institute of Semiconductor Physics, SO AN SSSR, Novoslblrsk (Institut fizikl
poluprovodnilcov SO AN SSSR)
TITLE: Investigation of the recombination emission ofS!~dmlum sulfide subjected to electron
excitation ? 1 -7
SOURCE: Fizilia tverdogo tela, v. 8, no. 5, 1966, 1461-4466
TOPIC TAGS: recombination emission, cadmium sulfide, electron excitation, semiconductor
crystal, emission spectrum
I ABSTRACT: The purpose of the present work is the investigation of the qpectrum and the
Idnetics of recombination emission (RE) of unalloyed CdS single crystalst'gubjected to excitation
by a pidsed beam of high-energy (200--400kev) fast electrons. It is found that the green band
is present on irradiated and nonirradiated specimens, moreover, after irradiation the peak of
the green band shifts toward the short wavelengths and the half-width of the band decreases.
No substantial variations were observed in the intensity, the half-width, or the peak position
of the red band of the RE spectrum after irradiation. These results preclude considering some
Card 1/2

-1/3403/3404
ACC NR:
Ap6o37003 61~iC~ CODE: UR/0181/66/008/01
AUTMR: idiaynovskaya, V. V.; Smirnov, L. S.
sk (Ins~itiat fizi-~
-QRG: Institute of Physics of Semiconductors, SO AN SSSR, Novosibir
oluprovodnikov SO AN SSSRY.
nteraction between radiation defects and dislocations in germanium
TITLE: I
SO'LrACE: Fizika tverdogo tela, V. 8, no. 11, 1966,'3403-34o4
TOPIC TAGS: crystal defect, crystal dislocation phenomenon, germanium semiconductor,
radiation effect, plastic deformation
ABSTRACT: To deiermine conditions for the recovery of the initial properties of ger
manium following irradiation, the authors observed the motion of dislocations during
irradiation of germanium by a flux of 3.5-Mev electrpns. p-type germanium with
resistivity 5 ohm-cm and initial dislocation density 103 Cm72 was subjected-to
plastic deformation in vacuum at 700C to introduce dislocations. To protect the in-
troduced dislocations fi~om impurities, the samples were coated with gold prior to
deformation. The dislocation position was determined.by an etching method. The
tests showd that irradiation caused a definite motion of the etch pits relative to
~6 e initial position (in the [111] direction), evidencing the'climbing of the dis-
th
locations as they absorb vacancies or interstitial atoms. The average climbing dis-
tance was -20 p, corresponding to absorption of 1012 atoms per unit dislocation
length. The dislocations were displaced by interaction vith point defects only at
Card V2

GAW,ICHKOV, Fedor Stepanovich; SHILIN, Boris Alekseyevich;
LYAKHOVP G.M., kand. tekhn. nauk, retsenzent; a
~ ~4011
IL.V,, otv. red.
[Miner of horizontal and inclined workings] Prokhodchik
gorizontalInykh i naklonnykh gornykh vyrabotok. Moskma,
Nedra, 1965. 235 P. ('PIIRA 18.7)

SMIRNOV, L.Y.; SABETSKIY, N.I.; MEZURITSKAYA, K.P., tekhnicheskiy redaktor.
[Radio vision; aeronautical panoramic radar] Radiovidenie; samoletnyi
panoramnyl radiolokator. Moskva, Voennoe izd-vo Ministerstva. oborony
Soiuza SSR, 1954. 56 p. (MLRA 8:1)
(Radar In aeronautics)

Subject : USSR/Aeronautics - training AID P - 4597
Card 1/1 Pub. 135 - 9/23
Author Smirnov, L. V., Eng.-Lt. Col.
Title Training of navigators in the ground trainer prior to
the bombing flight in overcast.
Periodical Vest. vozd. flota,3,~3, 45-50, Mr 1956
Abstract Detailed description of a simple bombing ground trainer
for the training of navigators in bombing under adverse
weather conditions. The aiming procedure is also
described. One photo, 2 sketches. The article is of no
particular interest.
Institution : None
Submitted : No date

SY10NOV, L. V.
"The Use of Dituirdnous Co=ositions and Cold Filling Corq)oimds for Cable Couplings,"
"Operation of Cable Networks" (Eksploatatsiya kabeley i kabel'nykh setey), Gosenergoizdat,
1949, 384 Pp.

SMIRNOVI L.V.; GORITSKIY, A.V., radaktor; SAVIF, M.M., redaktor;
'-'.'-ftg6ftiKOVA, Z.A., tekhnicheakiy redaktor.
[Londing rock while driving vertical mine shafts] Pograska
porody pri prokhodke vertikallnvkh stvoloy shakht. Moskva,
Uglatekhizdat. 1955. 48 p. NT.RA 9:4)
(Coal mines and mining)

T . * I
, "'? 11 ~' - " 1. r .. , ~?14. -! . I
~:-- . - " -. ~ L :" I ~ , -I
V-- -- , - , -- -)~' I'-;-. - ' '-- j_ ~_ __ 1' ~)
r-- _1~ If-'L, -- L 0, -*.-. t 3 . -'_ 'jj . 11, - '0.
- - Z~ ~ ~ . . - - I - ~ . 1, ; 1: 5,
i ~- -i
9. Monthl List of Russian Accessions, Library of Congress, A-.1 ~"~+ -19V, Uncl.
2

IVANOV, 4,Z.; SMIRNOV. L.V.
Characteristics of colorimetric glass from different sources. Sakh.prom.
27 no.8:31-33 Ag 153. (KI-RA 6:8)
1. Leningradskiy tekhnologicheskiy institut pishchevoy promyshlennosti.
(Glass) (Sugar--Analysis and testing)
J.

IVANOV, S.Z.: SHIRNOV, L.V.; KAMINSKATA, A.B.
standardization of the technical unit of chromaticity. Sakh.prom.
31 no.3:23-25 Mr '570 (MLMA '10:4)
1. Imeningradekly takhnologicheekly institut pishchavoy promyshlen-
nosti.
(Sugar-Analysis and ten %g)'(Celor measumment)
:4 ,

- 1- ...
FILIPPOVA, Ye.S.; YASOV, V.G.1 MUSIYFMO, I.A.; ARTSIMOVICH, G.V.;
EPSHTEYN, Ye.F., prof., doktor tekbn.naukj- USENKO,A.P.;
SIRIK, V.F.; SMIRNOV STONIYAN, A.Ya.,
___ , L.V., atv. red.; KW
reid. izd-va,--NM5EiA-,V.V., tekhn. red.
(Combination drilling of holes with hydraulic drills) Udarno-
vrashchatellnoe burenie skvazhin gidroudarnikami. Moskva
Gosgortekhizdat, 1963. 83 P* (Boring) (MIRA 16:5~

SMIRNOV, L-V. (Leningrad)
"The Simulation of Biological Phenomena"
Report presented at the 3rd Conference on the use of Mathemetics in Biology,
Leningrad University, 23-28 Jan. 1961.
(Primeneniye matematicheskikh Metodov v Biologii. II, Leningrad, 1963 PP 5-11)

SMIRNGV, L*V*
Model study of biological phenomena. Prim. mat. metod. v
biol. no.2:33-36 163. (MIRA 16:11)

USSR/Solid State Physics Mechanical Properties of Crystals E-10
and Polycrystalline Compounds.
Abs Jour Referat Zhur - Fizika, NO-5, 1957, 11938
Author Smirnov, L.V., Sadovskiy, V.D.
Inst
Title Investigation of the Reversible Temper Brittleness of
Structural Alloyed Steels.
Orig Pub Probl. metalloved. i term. obrabotok, Moskova - Sverdlovsk,
f4ashgiz, 1956, 120-140
Abstract A study -was made of the influence of the effect of the fol-
lowing factors on the development of reversible temper
brittleness: prolonged high temper, preliminary reheating,
and plastic deformation in the austenitic state. An expla-
nation is ptoposed fro the obtained results, and there
practical significance is indicated, particularly'With res-
pect to possible methods for improving the structure of
overheated steel. Bibliography, 6 titles.
Card 1/1

SOV/ 137-57- 10-20073
Translation from- Referativnyy zhurnal, Metallurgiya, 1957, Nr 10, p 233 (USSR)
AUTHORS, Smirnov, L.V,,. Sadovskiy, V.D.
TITLE, The Structural Mechanism of Transformations During the
Heating of Steel (K voprosy o struktUrnom mckhanizine prev-
rashcheniy pri nagreve stali)
PERIODIGAL~ Tr. In-ta fiz. metallov. Ural'skiy fil. AN SSSR, 1956, Nr
17, pp 94-110
ABSTRACT. An examination is made of the structural mechanism of the
formation of austenite in the heating of steel. The possibility
of nondiffusive transformation of martensite into austenite
with heating, by suppression of the d-iffusive processes of de-
composition (through raising the rate of heating, or by alloy-
ing), in a fashion similar to the supercooling of austenite to
the martensite point on cooling, is qualitatively proved. Grad-
ient heating followed by structure study is used on specimens
of 37KhNZA steel to investigate austenite formation. It is
Card I/Z shown that austenite formation may proceed either by a diffusive

SOV/ 137-57- 10-20073
The Structural Mechanism of Transformations During the Heating of Steel
reaction of ferrite and carbides or by an intermediate process with partial
precipitation of the C from the martensite, in which case the residual a solu-
tion of the alloying elements undergoes a "non diffusive" ordering transform-
ation, or by a truly nondiffusive reversible martensitic transformation.
Various transformation mechanisms may come into play, depending upon
the conditions of heating.
A. Z.
Card 2/2

"I

%k
Jp~

---- -------

E-V AbO
NOV WOLI, 0 S

Auenchinj...:O)'The variation ofah as unction of the test-)
a f
Ingtemp. wasdetil.In theraugeol +140 to -200*.
San to decrease Into the:brlttletess range. at W when hoi-
rolled and-at .+.100' when.h6tiolled_ Conclusion'. - Hot,
'),
*
reversible and irreversible tem
mech, Wnrktng rodumd both
-per brittleness providin
of austenite was Wtan
rec6sta
.
'a
nuted. Both iYpes 0 brittleness are sfinilar. Or :s but
f
lull
Wed by dlfferinl causes.
7 7.

itiatiall Steel on the appear-
erl v,alwalovaluly
AnCa d revviritible -9 fWAIllux
D. Trody-ImI.. FL-. Hddr-,.7TIU3
-S -65 -~~Thc effect of fittmo~
R.. Met. FirW 1956, No,18j'57 a.
gm=br tex'fitnE of h ed-st"Is.bittlic-appearince of
Wtenapervalcii
3
:.lowing tests were madewith st, _37.KhN,
'
d been oil-
h h
hi
R
b
1
ed
e
d

c
a
ece
a
str.):
s groun
fri p m w
) W
(
g
quenched fiiiin 13W*,were heated with anelea. currenrat the
rate.of 300o/sec.'so that the temp. at the pointed edge was at
1360* above the Acrm,-Ac~ crit. points. :-The hardness ff,,~,
'
the macro-
:evenlk spaced sections was-detil. and
at_-U
and micrograins at the saine sections examd.. Theffz, of the .
71" first- 14 SeCtiorm (froin thi. wide edge) where none,of the:-:
a -Y onim ri-occurred *aA'3A4l'X ereas that 4,

do wh
tmad
of the~sections 0~12 wai 52-40 X. - The m=ostructure W)
j of sectimm I-w-10 rcmWncd coarse, unchanged, wbem3 that of -
ISKtion IP-12,,chamed abmptly and couipletely luto a finer

d'
ond
o
res
) TI
abo
A
itn
tr
l
C
r
ve
ucture Re. c
t
ne
c.
p
gra
s
p~
-(
gradual change, at fint aum
ted
k
h
39O) indi
x
ca
a
=
rogm
m
ne ins
!viewing of martetisite, then the appearance of at

ginins. (abovii At At 5ect 5)
~'austeidte. between the origin
finally the forWatiou of an unarlented network of u c-

Z,
n.
like'rautedsite (section. 12). -The processes of.recryst
(cfi
could be!'
the move recent theories
ex
lai
ed only b
.
n
y
p
.!Arkharoli.-tti4.,.C.A~44;-4847tti. ~ The abrupt change train
'
s
;coarse taIne-graltim itmettires correspoiided to Chernov
'

tpoInt.b (cL rit. temp. be-:
C.4. 48.'12191) defined is that c
Le thb strue- I
'low which the'fractwe surface-did not change

... ... ,
we c
;tam did itht change and abdvi which the struct
In

Preclabi :.For steel 37KhN3&.this W t
ap
ain
W* 61
ca
1300* and th a
il t
h
a
e
r
in
g
Wem quenc
iquenched,front OW and-1100 w4sAd,and-17 lc_g./sq_ c1--
;
'
i
4
ef
. and then quenched In *
tempeied for I be; it 60
d

.5 $in
en

q

SOV/124-58-11-13627
Translation from: Referativnyy zhurnal, Mekhanika, 1958, Nr 11, p 233 (USSR)
AUTHORS: Sadovskiy, V. D. Malyshev, K. A. Sokolkov, Ye. N. , Smirnov, L. V.
Bogacheva, G. N. Biryulin, V. T. Petrova, S. N.
TITLE: The Influence of High- temperature Plastic Deformation on the Temper
and Aging Brittleness of Quenched Steels (Vliyaniye plasticheskoy
deformatsii pri vysokikh temperaturakh na khrupkost' pri otpuske i
starenii zakalennykh staley)
PERIODICAL: V sb. : Issled. po zharoprochn. splavam. Vol 2. Moscow, AN SSSR,
1957, pp 76-91
ABSTRACT: As a result of tests it was found that the brittleness developed upon
aging of austenite steel of the 60Yh4G8N8V type, as well as upon aging
of industrial high- temperature steel, can be held down through the
application of a combined thermom -echanical. treatment consisting of
the quenth.--hardening of a plastically deformed nonrecrystallized
austenite. The authors explain the effect of the thermomechanical.
treatment by the sharp Localization of the deformation, which at
elevated temperatures proceeds along the grain boundary, which leads
Card 1/2 to a reduction In the unfavorable effect of the phases that separate out

SOV/IZ4-58-11-13627
The Influence of High- temperature Plastic Deformation (cont. )
along the boundaries during the tempering and contribute to the development of
the brittleness.
D.M. Vasillyev
Card 2/2

SOV/126-6-2-12/34
AUTHORS: Sokolkov, Ye. N., Smirnov, L. V. and Petrova, S. N.
r
TITLE: Influence of The al Treatment Under Conditions
of Forging on the Impact Strength of Alloy Steels
(Vliyaniye termomekhanicheskoy obrabotki v usloviyakh
kovki na udarnuyu vyazkost' konstruktsionnykh
legirovannykh staley) -
PERIODICAL: Fizika Metallov i Metallovedeniye, 1958, Vol 6, Nr 2,
pp 276-280 (USSR)
ABSTRACT: In earlier work (Refs-1-3) it was established that
combination of hot rolling of steel in the austenitic state
~viba a haidening 17egi~w 9.kA as to eliminate recrystallisation of
austenite enables to reduce the drop in impact stren6th
after tempering at temperatures at which temper
brittleness develops. The authors considered it of
interest to study the effect of such "thermo-mechanical"
treatment under conditions of free forging. The experi-
ments were effected on the commercial steels 37E]uNZA and
35KhGSA. As blanksl beams of 20 x 20 x 200 mm. were used;
the forgina- was effected by means of a pneumatic hammer
with a reduction of 20%. FoF differing regimes vieSe
Card 1/4 used, namely: heating to 1150 C, cooling down to 950 C,

SOV/126-6-2-12/34
Influence of Thermo-mechanical Treatment under Conditions of
ForGing on the Impact Strength of Alloy Steels
forging, quenching; heating to 11~0 00. forging, quenchin~~;
heating to 11500C, cooling to 950'C, forging, soaking in
a fugnace (1150 C for 5 minutes), quenchin6; heating to
1150 0, quenching. The cooling to 950 C was applied as
a means of impeding possible recrystallisation during
forging. For the same reason the time -necessary for
obtaining the desired reduction was reduced to the
possible minimum and amounted to 4-5 secs which tiras
followed immediately by quenching. After quenching,
standard specimens of 10 x 10 x 60 mm were pro--iuced by
grinding for impact bend tests. All the specimens were
tempered at a temperatuse at which reversible temper
brittleness occurs (550 C for four hours). On the
finally machined specimens a notch 2 mm wide 7 2 mm deep
with a curvature radius of 1 mm. at the bottom of the
notch was produced. The obtained imDact strenSth and
hardness values are given in a table, p 276. Micro-
structure photographs and photographs of fractures are
reproduced. It was found that "thermo-mechanical"
Card 2/4 treatment under conditions of forging as ivell as under

SOV/126-6-2-12/34
Influence of Thermo-mechanical Treatment Under Conditions of
Forging on the Impact Strength of Alloy Steels
conditions of rolling brings about a reduction of the
sensitivity of the steel to develop reversible temper
brittleness. In both cases this effect is associated
with the localisation of tht deformation along the
boundaries of the austenite grains of the,initial heating,
distortions in the crystal la-Lt~ce of the intergranular
transient zones (which are cofse-rved after hardening)
and the thereby caused change in the form of the phases
and compounds which are responsible for developing
temper brittleness. The here described effect of
therino-mechanical treatment can also be observed in other
types of hobwarking as, for instance , stamping and extrusion,
under conditions such that recrystallisation. of work-
hardened austenite is prevented.
Card 3/4

SOV/126-6-2-12/34
Influence of Thermo-mechanical Treatment Under Conditions of
Forging on the Impact Strength of Alloy Steels
There are 3 figures, 1 table and 4 references, 3 of
which are Soviet, 1 German.
ASSOC IATI 0-111: Institut f iziki metallov Ural I skogo f iliala AN SSSIR
(Institute of Metal Physics, Ural Branch of the
Ac.Sc. USSR)
SUBMITTED: November 19, 1956.
Card 4/4 1. Steel-Mechanical properties 2. Steel--Temperature factors
3. Steel--Test results

SADOVSKIY, V.D.; BOGACEEWA, G.N.; SMIRROV, L.V.; SOROKIN, I.P.; KOMPAIWTSZV,
N.A.
Investigating phase recrystallization in titanium. Piz. met. i
metalloved. 10 no-3:397-403 S 160. (MIRA 13:10)
1. Institut fiziki metallov AN SSSR.
(Titanium--Metallography)
(Phase rule and qquilibrium)

9,14, 1~ 1,00 26567
g -75-00 cj/,o 116J) 1~%2_
S/126/61/012/002/019/019
E073/E535
AUTHORS: Sadovskiy, V.D., Rodigin, N.M., Smirnov, L.V.,
Filonchik, G.M. and Fakidov, I.G.
TITLEi On the influence of a magnetic field on the martensitic
transformations in steel
PERIODICAL: Fizika metallov i metallovedeniye, 1961, Vol.12, No.2,
pp-302-304
TEXT: The authors investigated the effect of a magnetic
field on martensitic transformations using specimens 3 mm. dia.,
50 mm long,of steel JXa H (9Kh2N) (0.9% C, 1.83% Cr, 0.53% Ni,
0.27% Si, 0.30% Mn, 0.01% S, 0.018% P). These specimens were
quenched from 850 and IOOOOC in oil (so that they contained
respectively 11 and 37% residual austenite) and were then
subjected to a single magnetization by means of super-strong
magnetic field pulses (200-350 kOe, 3000 c-P.s.). Magnetic
measurements by a ballistic method did not show any increase in
the martensite. Experiments at liquid nitrogen temperature also
did not reveal a decrease CAbstractor's Note: Printing error for
increase] in the quantity of residual austenite as a result of
Card 1/4

26567
On the influence of a magnetic field ... S/126/61/012/002/019/019
E073/E535
applying the magnetic field; only the usual increase in the
quantity of martensite corresponding to deep cooling was observed.
An increase in the number of magnetization cycles to five also had
no influence on the results. Thus, it can be concluded that in
the general case pulse magnetization even with very strong fields
does not produce transformation of residual austenite in quenched
steel. Further experiments were made with steel30)(Wa3 (50KhN23)
(0-52% C, 1.49% Cr, 22.85% Ni, 0.3% Si, 0.19% Mn, o.o68% P).
Quenching of this steel from 12000C yields a purely austenitic
structure at room temperature. Martensitic transformation begins
at about -100*C and at liquid nitrogen temperature the residual
austenite amounts to 40-50%. Fifty pulse magnetization cycles
(40-50 kOe) during cooling showed only a very slight effect on the
quantity of martensite. Further experiments were carried out on
the assumption that the martensitic point is lower for fine grained
austenite than for coarse grained. Therefore, another series of
experiments was carried out in which steel 50KhN231was water
quenched from 1200% and cold rolled with a reduction of 60% and
then again water quenched from 850, 900, 950 and IOOOOC; this
Card 2/4

26567
On the influence of a magnetic field ... S/126/61/012/002/019/019
E073/E535
material was used for producing magnetometric specimens. At room
temperature all the specimens had a purely austenitic structure
but their grain size differed. Cooling in liquid nitrogen
revealed that specimens quenched from 850, 900 and 9500C contained
I to 3% martensite but the coarser grain specimens,whi6h were
originally quenched from 1000*C, contained 20 to 30% martensite
after cooling in liquid nitrogen. However, pulse magnetization
at liquid nitrogen temperature produced intensive austenite to
martensite transformation even in the fine grained specimens
quenched from 850 to 9000C. The increase in the number of magnet-
ization cycles did not have a great influence. It is concluded
that pulse magnetization can intensify austenite to martensite
transformation. In the investigated case, the austenite was
artificially stabilized by its fine grain size and is in a super-
metastable state at the liquid nitrogen temperature, being under-
cooled considerably below its normal martensitic po�nt. Activation
of the transformation under the effect of a magnetic field is
probably due to magnetostriction effects associated with the
presence of a certain quantity of the magnetic phase. The problem
Card 3/4

26567
On the influence of a magnetic field ... S/126/61/012/002/019/019
E073/E535
requires further study. There are 3 figures and 6 references:
4 Soviet and I English which reads as follows: Metal treatment
and Drop Forging, 1960, 27, No.18o, 362.
ASSOCIATION: Institut fiziki metallov AN SSSR
(Institute of Physics of Metals AS USSR)
SUBMITTED: May 22, 1961
Card 4/4

SHAPIRO, N.I.; SMIRNOV, L.V.
Efficient method of Tjrr:;-.Pring a solid metal open-hearth furnace
charve. Zi no.g-.~852 S 161. (MIMAI 14:9)
1. Giprostale.
furnaces-Equipment and supplies)
(Scrap metals)

U165
S/181/62/004/012/016/052
B100102
AUTHORS: Bogoroditskiy, N. P., and Smirnov, L. V.
TITLE: Problem of the anomalous polarization of titanium
dioxide (rutile)
PE,-,IODICAL: Fizika tverdogo tela, v. 4, no. 12' 1962, 3418-3421
TEXT: In studies of the anomalous polarization of rutile ceramics
(G.1. Skanavi and A.I. Demeshina, ZhETF, XIX, 3v 949; Ya.M. Ksendzov)
ZhTP, XX, 1, 117, 1950; L.I. Reymerov, ZhTF, XXVI, 3, 1960; Ya.M. Ksend.zov,
'Izv. AIN SSSR, ser. fiz., 22, 3, 287, 1958) the ohmic conductivity was
assumed to be low enough in comparison with the capacitive component for...
it to be 'heglected. Here the correctness of'this assumption is checked.,"
The ele'ctric properties (F_, tan6, Eeff ) ok identically prepared TiO2 . 1
specimens containing Nb 0 'impurities, with,,Ag-Ag and Ag-In electrodes, as
2 5
well as the volt-ampere characteristic of th~ Ag-TiO 2 contacts were
investigated. It became evident that'the high-resistance contact layers
must be considerqd. What are called the Anomalous effecls are attributed*
Card.1/2

s/126/62/013/003/007/023
The effect of .... F,193/F,383
of test pieces was subject to the same heatin cooling cycle
without, however, plastic deformation at 800 C. Creep tests
0
were carried out at 500 C on test pieces of each series. The
results are reproduced in Fig. 3, where the stress
2
(o,, kg/mm ) is plotted against time-to-rupture hrs),
P
the continuous and broken curves relatIng, respectively, to
CJ
material subjected to TDIO and to the pilot_ I est pieces. The
rate of steady creep amounting to 1.1 x 10 0/0'/hr for the pilot
test pieces was 3.5 x 10 %/hr for material subjected to TMO.
Since it could be postulated that the higher creep resistance of
-5
specimens subjected to TMO was due to their higher hardness 0 i
(100 BHN as compared with 60 BFIN of nickel quenched from 800 C)
a supplementary series of tests was carried out on specimens given
0
the following treatment: heatin 9 to 1~ 100 C.; quenching;
250% reduction by rolling at 300 C and 12 hours~annealing at
500 OC. The results are reproduced in a table. It-will be
Card 2/4

R0,14ANOV SIURNOV L.V.j SADOVSKIY, V.D~," VOLKENSHIPEY09 N.V.
I , IV, 111. -
I In
Criti!!a'l current of a dispti,se supen,onductl g phaee ob-~ainfid
during aging. Fiz. met, i metalloved. 20 ncJ1455-458 S 165.
a
(~Eru 18:21)
1. fizili metallm, AN SSSR.

5OKh2N22' 0.49 21. 9 2.64 0.26
j9K 0.52 22.8 1.4S 0-19
5onl2NI6 if 0.52 16.44 2.01 0.47 0.63,
50Kh2N3 0.51 3.21 2.00 0.35 .0011
2e. 5u N 12 4 M 2,
N30 0.21

0.06 24.10
29.72 ~.0*22
0.15 .0.06 2. 1:6
-

Khl2
1.35
12.3
~0.19 0.92
.1.09 1.37 .~,0.30 0.26

U12 1.25 os2, 0.33 0.26

7t

Card, 3~3.

L 4186-66 rdT(m)/b-PF(c) M/EWP(Z)/EWP(b)/EWA(c) IJP(d)
ACCESSION NR: AP5016535 MJW/JD UR/0126/65/019/006/0932/0933
AUTHOR: Fokina, Ye. A,,* Smirnov h. V.; Sadovskiy, V. D
Pr#
Y'11 5-
TITLE: On the problem of the effect of a constant magnetic field on the martensitd
transformation in steel
SOURCE- Fizika metallov i metallovedeniYe, v. 19, no. 6, 1965, 932-933
TOPIC TAGS: martensitic trandfomation,,constant magnetic field,-strong magnetic
field, liquid helium, steel
ABSTRACT: At the Institute of Physics of'Metals experiments were performed on
5OKhN23 steel in a slowly increasing then constant (for 6 min) ma'gnetic field of 7
40 kOe 1~ a solenoid with a superconducting winding at liquid helium temperature.
Without the magnetic field,.this steel does not undergo a martensite transformation
on cooling to -1960C, but cooling to the liquid helium temperature causes the formi-:-'
tion of 8-9% martensite. When the field was applied, an additional 12% martensite~_*
was formed. Similar experiments with the same steel carried out at the Physics
Institute gave analogous results*. In another steel, 50MR22) which no martenT:',__
site is formed on cooling in liquid helium, the application ofirconstant magnetic L_-I.
Card 1/2

L 26646-66 EWT(m)/EPF(n)-2/T/9WP(t) IJP(c) JDIWWIJG
:ACC NR: AP5025333 SOURCE CODE: 'UR/0126/65/020/003/0455/0458
7 L
'1AUTHOR: Romanov, Ye..P.;.Smirnov..,L. V.: Sadovskiv.
V 1) Volkenshteyn, N.
jORG: Institute of Metal Physics', AN SSSR (Institut fiziki metallov.AN'SSSR)
iTITLE: Critical current of the superconductive dispersion phase obtained during
4n-ing
!SOURCE: Fizika metallov i metallovedeniye,.v. 20, no. 3, 1965, 455-458
I zirconium base alloy, niobium containing
TOPIC TAGS: martensitic transformation
lalloy p SuPerconductivityy metal aging, solid solution,, plastic deformation
metal heat treatment, current density
,ABSTRACT: A nonsuperconductive alloy at 4.20K was used which could separate a
;superconductive dispersion phase during the process of thermal treatment or aging.
~The alloy used waa zirconium with 4% niobijHLylAfter preparation, superconductivit
Y,
!was obtained eveti~f -tersbort thermal treatment at a temperature of 5000C--)
Maximum critical density is obtained after heating the sample for 2~ hourt,: Furthe
heating results in a decrease of critical current,density.. When heating the
zirconium-4% niobium alloy a supersaturated niobiumiZ-solid solution is obtained''
from the stable Id'-solid solution as a result of martensite transformation.
UDC: 537.312.62
Card 1/2
77

L 26646-66
ACC NR: AP5025333

~M~/E~i~d)/EWP(t) Mkc)
'"'CC NRI AP6005132 SOURCE CODE: UR/0126/66/021/001/0017/0020
4,UTHOR: Romanov, Ye. P.; Sadovskiy, V. D.; Volkenshter, N. V.; Swirnov, L. V.
ORG:. Institute of the Physics of Metals, AN SSSR (Institut fiziki metallov)
TITLE: Disruption of superconductivity in an allolykth a disperse superconducting
phase - 1ZL I t q q I t~
SOURCE: Fizika metallov i metallovedeniye, v. 21, no. 1, 1966, 17-20
ITOPIC TAGS: superconductivity, zirconium alloy, magnetic field, solenoid
ABSTRACT: This is a continuation of a previous investigation (Romanov et al. FMM,
i1965, 20, 3) with the difference th t i t tain indings on the disruption
; Zihpresen a c f
of superconductivity in the alloy 4 47,jN-4 weight following the decomposi-
on il 3a
tion of supersaturated solid soj.uti ngJ udinal magnetic field generated by
g
0
means of a superconducting solenoid at 4.2 ~Khe current was introduced at a smoothly
increasing rate into the specimens by means of a semiconductor amplifier and the dis-
ruption of superconductivity was recorded by means of an automatic-recording millivolt
meter. It is found that for the alloy investigated the transition from superconducting
to normal state is abrupt in the absence of the magnetic field and increasingly smooth
the greater is the intensity of the magnetic field applied. Plotting of the curves of
electric resistance as a function of the current introduced (Fig. 1) revealed that